Status of SPARC Undulator

Slides:



Advertisements
Similar presentations
Stephen Benson U.S. Particle Accelerator School January 28, 2011 Establishing Lasing in the FEL* * This work was supported by U.S. DOE Contract No. DE-AC05-84-ER40150,
Advertisements

Two-dimensional Effects on the CSR Interaction Forces for an Energy-Chirped Bunch Rui Li, J. Bisognano, R. Legg, and R. Bosch.
1 Optimal focusing lattice for XFEL undulators: Numerical simulations Vitali Khachatryan, Artur Tarloyan CANDLE, DESY/MPY
Velocity bunching SPARC Daniele Filippetto on behalf of SPARC team.
J. Rudolph, Helmholtz-Zentrum Berlin EuCARD 2nd ANNUAL MEETING Slice emittance measurements at the ELBE superconducting RF photoinjector.
Bunch Compressor 3 Torsten Limberg for Frank Stulle et al.
SCU Magnet Modelling: Tolerances and Beam Trajectories Ben Shepherd Superconducting Undulator Workshop RAL, April 2014.
Stephen Benson U.S. Particle Accelerator School January 17, 2011 The FEL as a Diagnostic* * This work was supported by U.S. DOE Contract No. DE-AC05-84-ER40150,
Performance Analysis Using Genesis 1.3 Sven Reiche LCLS Undulator Parameter Workshop Argonne National Laboratory 10/24/03.
Isaac Vasserman Magnetic Measurements and Tuning 10/14/ I. Vasserman LCLS Magnetic Measurements and Tuning.
X-Ray Diagnostics for the LCLS Jan , 2004 UCLA.
A U.S. Department of Energy Office of Science Laboratory Operated by The University of Chicago Argonne National Laboratory Office of Science U.S. Department.
DELTA Quadrant Tuning Y. Levashov, E. Reese. 2 Tolerances for prototype quadrant tuning Magnet center deviations from a nominal center line < ± 50  m.
R. Bartolini, John Adams Institute, 19 November 20101/30 Electron beam dynamics in storage rings Synchrotron radiation and its effect on electron dynamics.
Magnetic Compression of High Brightness Beams: Survey of Experimental Results Scott G. Anderson ICFA Sardinia July 2002.
Simulation of direct space charge in Booster by using MAD program Y.Alexahin, N.Kazarinov.
1 BROOKHAVEN SCIENCE ASSOCIATES Hard X-Ray Wiggler Sources at NSLS-II Oleg Chubar X-ray source scientist, XFD, NSLS-II Workshop on Preparation of High-Pressure.
The impact of undulators in an ERL Jim Clarke ASTeC, STFC Daresbury Laboratory FLS 2012, March 2012.
Transverse emittance Two different techniques were used to measure the transverse emittance. The multislit mask in the injector 9 MeV Quadrupole scan for.
Y. Ohnishi / KEK KEKB LER for ILC Damping Ring Study Lattice simulation of lattice errors and optics corrections. November 1, 2007 Y. Ohnishi / KEK.
PS Booster Studies with High Intensity Beams Magdalena Kowalska supervised by Elena Benedetto Space Charge Collaboration Meeting May 2014.
DTL: Basic Considerations M. Comunian & F. Grespan Thanks to J. Stovall, for the help!
Two Longitudinal Space Charge Amplifiers and a Poisson Solver for Periodic Micro Structures Longitudinal Space Charge Amplifier 1: Longitudinal Space Charge.
FCC electron cloud study plan K. Ohmi (KEK) Mar FCC electron cloud study meeting CERN.
Beam Dynamics and FEL Simulations for FLASH Igor Zagorodnov and Martin Dohlus Beam Dynamics Meeting, DESY.
Optics considerations for ERL test facilities Bruno Muratori ASTeC Daresbury Laboratory (M. Bowler, C. Gerth, F. Hannon, H. Owen, B. Shepherd, S. Smith,
Emittances Normalised r.m.s. Emittances at Damping Ring Extraction Horizontal Emittance (  m) Vertical Emittance (  m)
Kiyoshi Kubo Electron beam in undulators of e+ source - Emittance and orbit angle with quad misalignment and corrections - Effect of beam pipe.
By Verena Kain CERN BE-OP. In the next three lectures we will have a look at the different components of a synchrotron. Today: Controlling particle trajectories.
RMS Dynamic Simulation for Electron Cooling Using BETACOOL He Zhang Journal Club Talk, 04/01/2013.
ILC Positron Production and Capturing Studies: Update Wei Gai, Wanming Liu and Kwang-Je Kim Posipol Workshop, Orsay, France May 23-25, 2007 Work performed.
Beam dynamics simulations with the measured SPARC gun- solenoid field G. Bazzano, P. Musumeci, L. Picardi, M. Preger, M. Quattromini, C. Ronsivalle, J.
Numerical Simulations for IOTA Dmitry Shatilov BINP & FNAL IOTA Meeting, FNAL, 23 February 2012.
Lecture 1: Synchrotron radiation Lecture 2: Undulators and Wigglers
Lecture 1: Synchrotron radiation Lecture 2: Undulators and Wigglers
Some Simulations for the Proposed Hard X-Ray Self- Seeding on LCLS J. Wu J. Wu et al. Feb. 25, 2011.
Review of Alignment Tolerances for LCLS-II SC Linac Arun Saini, N. Solyak Fermilab 27 th April 2016, LCLS-II Accelerator Physics Meeting.
ILC Positron Production and Capturing Studies: Update Wei Gai, Wanming Liu and Kwang-Je Kim ILC GDE Meeting DESY May 30 – Jun2, 2007 Work performed for.
SIMULATION FOR TW LCLS-II Tor’s question on the undulator length in the TW FEL senario SASE FEL undulator length 9, 10, and 11:  9 – m, 10.
Magnetic Field optimization of EPU at TPS
Dielectric Wakefield R&D programme at Daresbury Lab.
Correlated Misalignments Studies for LCLS-II SC Linac
Update on e+ Source Modeling and Simulation
Status of the CLIC DR wiggler design and production at BINP
EUPRAXIA-PISA JUNE 2016 e-Beam-Laser
X. Ding, UCLA MAP Spring 2014 Meeting May 2014 Fermilab
Simulation of Luminosity Variation
A.Smirnov, A.Sidorin, D.Krestnikov
Primary estimation of CEPC beam dilution and beam halo
Electron Cooling Simulation For JLEIC
Status on Work for Splitter FS and Dilution System FS
Test of Optical Stochastic Cooling in CESR
LCLS Undulator Fiducialization
Undulator Tolerances for LCLS-II using SCUs
Yuhui Li How to edit the title slide
Experimental Overview
SCU Next Phase Meeting July 8, 2014.
Experimental Optimization and Characterization of Electron Beams for Generating IR/THz SASE FEL Radiation with PITZ. P. Boonpornprasert, G. Asova1, Y.
Relaxing Quads Roll Alignment tolerance
Phase Adjustments: K vs
PERMANENT MAGNET QUADRUPOLE FOR THE LINAC 4 CCDTL
Status of FEL Physics Research Worldwide  Claudio Pellegrini, UCLA April 23, 2002 Review of Basic FEL physical properties and definition of important.
Undulator Line Design Liz Moog, Advanced Photon Source April 24, 2002
Laser Heater Integration into XFEL. Update.
Studies on orbit corrections
Gain Computation Sven Reiche, UCLA April 24, 2002
LCLS FEL Parameters Heinz-Dieter Nuhn, SLAC / SSRL April 23, 2002
Achieving Required Peak Spectral Brightness Relative Performance for Four Undulator Technologies Neil Thompson WP5 – 20/03/19.
Linac Design Update P. Emma LCLS DOE Review May 11, 2005 LCLS.
New VUV-FEL Simulation results
Presentation transcript:

Status of SPARC Undulator F.Ciocci ENEA Fis-Mat

Undulator parameter set Periods 2.8 cm No of periods 77 Gap (nom.,min,max) 0.925,0.6,2.5 cm K (nom.,min,max) 2.145, 3.2, 0.38 Drifts between undulator sections 36 cm PM remanent field 1.3 T Blocks per period 4 Bock size (h x t x w)* 2 x 0.7 x 5 cm * H= height t= thickness, w= width

Electron beam parameters Beam Energy 150 MeV Peak current 100 A Energy Spread (slice) < 0.1 % Emittances (slice) 1 mm mrad Numerical codes used for FEL simulations PROMETEO (ENEA) PERSEO (ENEA) PARSIFEL (ENEA-codice semi-analitico.) GINGER GENESIS

FEL power evolution vs longitudinal coordinate z (lu = 2.8 cm, K = 2.1413, I = 100 A)

Mechanical tollerances Deflection of the undulator support structure, induced by the weight and by the attraction between the undulator surfaces, determined by the magnetic forces Misalignment of the undulator pole faces with respect to mid plane axis

Transverse misalignment of the undulator pole faces with respect to mid plane axis Misalignment of the undulator pole bars with respect to z axis

Combined effect of the misalignment and of the deflection due to the magnetic forces on the evolution of the FEL power Effect of the induced deflection and misalignment on the evolution of the power of the fundamental and higher order harmonics d= 10mm f = 5 mrad.

analysis of magnetic field errors We have performed a numerical simulation of the effect on FEL power behaviour of the magnetic field errors due to the magnetic blocks characteristics. We have assumed that the maximum deviation between the single block magnetization is 1% and 1° is the maximum deviation of the magnetization axis. Assuming that the magnetizations of the single blocks and the relevant orientations have gaussian distributions, we find, that they are characterized by the rms values

Pierce parameter conditions DT=k 0.3° C

Undulator Technical specifications Value of the on axis (peak) magnetic field B at a gap of 0.925cm 8.27 . 103 G R.M.S. relative peak magnetic field < 10-3 First field integral < 0.5 G . m Second field integral < 0.6 G . m2 Accuracy of the single period to maintain the Phase locking Dlu along the undulator < 20 mm

ACCEL Hybrid Undulator for DELTA

TIME SCHEDULE 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 Detailed Undulator design Construction and factory testing of the first Undulator Prototype Section Construction and factory testing of the 5 Undulator Series Sections ENEA Acceptance Test

Mechanical alignment of the sections Each section must foresee the necessary equipment to fulfil the following tolerances for the mechanical alignment of the complete undulator device Maximum Error of transverse positioning (vertical and horizontal) 50 mm Maximum Error of longitudinal positioning 50 mm Maximum error of angular alignment (f) 5 mrad Maximum error of angular alignment (q) 5 mrad Maximum error of angular alignment (y) 100 mrad

Sparc versus Sparx Current 2000 A Energy 1150 MeV Energy Spread 0.5 10-3 Emittances 1 mm mrad

Power vs. z